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Critical O(N) - vector nonlinear sigma - models: A resume of their field structure
High Energy Physics - Theory · Submitted 8 Nov 1993
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is proved that the only conserved quasi - primary currents are the energy - momentum tensor and the O(N) - Noether currents.
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The abstract, sentence by sentence
The classification of quasi - primary fields is outlined. It is proved that the only conserved quasi - primary currents are the energy - momentum tensor and the O(N) - Noether currents. Derivation of all quasi - primary fields and the resolution of degeneracy is sketched. Finally the limits d=2 and d=4 of the space dimension are discussed. Whereas the latter is trivial the former is only almost so.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The classification of quasi - primary fields is outlined. | contribution 0.96 | 0.73 | 0.07 | asserted 0.95 |
| s1 | It is proved that the only conserved quasi - primary currents are the energy - momentum tensor and the O(N) - Noether currents. | result 0.99 | 0.85 | 0.63 | asserted 1.00 |
| s2 | Derivation of all quasi - primary fields and the resolution of degeneracy is sketched. | contribution 0.86 | 0.82 | 0.09 | asserted 0.81 |
| s3 | Finally the limits d=2 and d=4 of the space dimension are discussed. | contribution 0.96 | 0.81 | 0.04 | asserted 0.92 |
| s4 | Whereas the latter is trivial the former is only almost so. | interpretation 0.72 | 0.43 | 0.05 | asserted 0.98 |
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Original abstract
The classification of quasi - primary fields is outlined. It is proved that the only conserved quasi - primary currents are the energy - momentum tensor and the O(N) - Noether currents. Derivation of all quasi - primary fields and the resolution of degeneracy is sketched. Finally the limits d=2 and d=4 of the space dimension are discussed. Whereas the latter is trivial the former is only almost so.
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3 arXiv papers cite this in 5 sentences
Papers citing it
Compares with it 2 papers
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We have also checked that the results agree with known results in the large \(N\) expansion [ref] .
Critical O(N) model to order $\epsilon^4$ from analytic bootstrap · Constraints from low spins · 1.00
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We presented the anomalous dimension in this way to draw an analogy with equations (61) and (63) of [ref] , which give the large spin expansion of the large $N$ anomalous dimensions of non-singlet and singlet operators in the critical $O(N)$ model [ref] .
On the Higher Spin Spectrum of Chern-Simons Theory coupled to Fermions in the Large Flavour Limit · Large Spin Expansion · 1.00
Cites it as background 2 papers
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Among the simplest and best known examples are the bosonic and fermionic (or Gross-Neveu) $O(N)$ vector models which are renormalizable field theories in the context of the $1/N$ expansion.[For reviews see [ref] .] These models exhibit critical behavior described by nontrivial CFTs with perturbatively calculable anomalous dimensions for all operators in their spectrum (e.g. [ref] ).
Singleton deformation of higher-spin theory and the phase structure of the three-dimensional O(N) vector model · Introduction and Summary · 1.00
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(See [ref] for a review, and e.g., [ref] for calculations of scaling dimensions in vector models related to this paper) or the large flavour limit of 3d QED and QCD (e.g., [ref] ).
On the Higher Spin Spectrum of Chern-Simons Theory coupled to Fermions in the Large Flavour Limit · Introduction and Summary of Results · 0.83
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